TiO_2对α-Fe_2O_3纳米微粒拉曼散射效应的影响

选取α Fe2O3和TiO2研究一种氧化物对另一种氧化物的拉曼散射效应。采用Sol gel方法制备纳米α Fe2O3/TiO2复合微粒,α Fe2O3粒径及含量分别为20nm、150nm和3%、6%、12%。制备过程中调节水解时的pH值和热处理温度,得到掺杂α Fe2O3粒子的不同晶型的TiO2纳米颗粒。Raman测量结果显示,α Fe2O3粒径越小、含量越高,TiO2对其散射效应的影响越大。不同的TiO2晶型对α Fe2O3纳米粒子的拉曼增强效应也不同。锐钛矿型及金红石型TiO2对α Fe2O3有一定的拉曼增强作用,当水解pH值较小时,得到板钛矿型TiO2,由于部分板钛矿型TiO2振动声子模的峰位与α Fe2O3的重叠,所以尚难观察它对α Fe2O3的拉曼增强效应。     

Reflection-absorption infrared spectrum of α-CO chemisorbed on polycrystalline tungsten

The infrared spectrum of chemisorbed α-CO on polycrystalline tungsten has been studied using ultrahigh vacuum techniques. The α-CO state has been spectroscopically resolved into two states, designated α₁-CO (wavenumber ～2128 cm^?1) and α₂-CO (wavenumber ～2090 cm^?1). α₂-CO adsorbs predominantly in the first stages of α-CO adsorption; α₁-CO forms primarily at high α-CO coverages at the partial expense of α₂-CO. α₁-CO is found to desorb at a slightly lower temperature than α₂-CO. Both α-CO states are postulated to involve sp-hybridized carbon which is bonded to the tungsten surface. These states have previously been detected in electron impact desorption measurements, where α₁-CO was shown to liberate CO⁺ and α₂-CO to liberate O⁺.     

Mechanical properties of novel forms of graphyne under strain: A density functional theory study

The mechanical properties of two forms of graphyne sheets named α-graphyne and α2-graphyne under uniaxial and biaxial strains were studied. In-plane stiffness, bulk modulus, and shear modulus were calculated based on density functional theory. The in-plane stiffness, bulk modulus, and shear modulus of α2-graphyne were found to be larger than that of α-graphyne. The maximum values of supported uniaxial and biaxial strains before failure were determined. The α-graphyne was entered into the plastic region with the higher magnitude of tension in comparison to α2-graphyne. The mechanical properties of α-graphyne family revealed that these forms of graphyne are proper materials for use in nanomechanical applications.     

On the dynamics of pulsating detonations

To understand the circumstances in which a pulsatingdetonation wave may prefer a low-frequency mode ofoscillation, and the implications this has formathematical modelling, the dynamics of a detonation waveare studied when the underlying linear stability spectrumconsists of at most two unstable modes. One mode α₁ has a period much larger than the time-scaleof particle passage through the half-reaction length inthe steady one-dimensional detonation; the second α₂ has a smaller period than α₁. Thequestion addressed in this paper concerns the long-timebehaviour of the pulsating detonation in the presence ofthe unstable modes α₁ and α₂. Westudy two general scenarios related to a crossing of theneutral stability boundaries traced out by α₁ and α₂. In all cases where the mode α₁ is unstable, the pulsating detonation emerges with alow-frequency, large-amplitude oscillation, regardlessof the relative growth rates of α₁ and α₂. Only in one case, where thehigher-frequency mode α₂ is alone unstable, isthe long-time nonlinear pulsation of high frequency. Inthis case, the amplitude of the oscillation issignificantly smaller than that observed in thelow-frequency oscillations. In all cases, the finalperiod of the nonlinear oscillation is closely related tothat of the relevant underlying linear mode.     

Dielectric properties of α-zirconium phosphate and its organic derivatives

Dielectric properties of compact discs of α-zirconium phosphate, α-zirconium bis(hydroxymethanephosphonate), in an- hydrous and monohydrated form, and of α-zirconium bis(carboxymethanephosphonate) were investigated, as a function of the temperature, at frequencies ranging from 30 Hz to 100 kHz and, in some cases, up to 2.5 MHz. In all the compounds a low frequency dispersion has been found and ascribed to polarization phenomena due to charge transfer through the compact discs. The comparison of the ?_∞ values of α-Zr(HOOCCH₂PO₃)₂, α-Zr(HPO₄)₂· H₂O and α-Zr(HOCH₂PO₃)₂· H₂O with that of α-zirconium pyrophosphate clearly indicate that orientation polarization is not present in these compounds. The dehydration of α-Zr(HPO₄)₂·H₂O and of α-Zr(HOCH₂PO₃)₂· H₂O is associated with an increment, at low frequency, of the real component of the dielectric constant and with a high frequency dispersion, due to relaxation of orientation polarization. Dielectric properties of α-zirconium phosphate are discussed on the ground of its crystalline structure.     

164Lu的三轴超形变核态的理论计算

用三维TRS(totalrouthiansurface)自洽理论对奇奇核164Lu的位能面进行了计算,计算结果与实验上得到的ε2=0.38基本一致,从而从理论上确认了164Lu是三轴超形变核,并且指出了存在三轴超形变带的两个组态. Total routhian surface in~(164)Lu nuclei is calculated according to the three dimensional Total Routhian Surface (TRS) theory. The result of the calculation is in agreement with the experiment. At the same time, two TSD bands could be assigned to the configuration(π\(1/2), α=1/2)(ν\(5/2), α=1/2), (π\(1/2), α=1/2)(ν\(3/2), α=-1/2).     

Relative thermoluminescence effects of alpha‐ and beta‐ radiation

Abstract

A study has been made of the relative thermoluminescence response to α- and β-radiation of six phosphors (two types of natural fluorite, CaF₂: Mn, CaF₂: Tb, CaSO₄: Mn and quartz) using samples which are thin compared to the range of the α-particles. The α- and β-radiations induce the same glow peaks, but at low doses (<100 rads) the TL response per rad of α-radiation (3.7 MeV) is less than that per rad of β-radiation in all the glow peaks studied. The α-efficiency ranges from 53 per cent for CaF₂: Mn to 2 per cent for quartz (110°C peak) at 3.7 MeV and decreases with decreasing α-particle energy. At higher doses (10⁶?10⁷ rads) the TL responses to α- and β-radiation become equal within 15 per cent; most of the glow peaks are in or near saturation at these doses. The higher the β-dose at which a peak saturates, the higher is the α-efficiency (at low doses) of that peak. The results support the interpretation that the α-efficiency is low because the phosphor is near or in saturation in the localized region near the α-path. This interpretation is given quantitative support by a theoretical calculation of the localized energy-density.     

α-Mg3Sb2的电子结构和力学性能

运用第一性原理研究了Mg-Sb合金中典型沉淀相α-Mg3Sb2的几何、电子结构和力学性能.结构优化得到的晶格常数和形成能与实验值符合很好.电子结构分析表明,具有半导体性质的α-Mg3Sb2带隙为0.303 eV,是间接带隙半导体.通过计算得到了α-Mg3Sb2的弹性常数,进而得到模量、泊松比等力学参数,对力学参数进行分析发现,α-Mg3Sb2有很好的延展性而塑性相对较差.通过对α-Mg3Sb2施加应变前后态密度的变化分析,发现对于六角结构的α-Mg3Sb2,与剪切模量相关的C11+C12,C33/2和与体模量相关的C11+C12+2C13+C33/2对体积变化不保守,而(C11-C12)/4和C44对体积变化保守.     

Die Reaktion11B(d, α)9Be im Energiebereich von 0,7 bis 2,2 MeV

Excitation functions were measured from 0.7 to 2.2 MeV for the α₀ -, α₁-, α₂- and α₃-groups at an angle ofθ _L=90°. Two broad maxima were found in all four cases, suggesting the existance of resonances in the¹³C-compound nucleus. A problem, however, arises, as the first maximum appears at a bombarding energy of 1.15 MeV for the α₀- and α₁-groups, whilst it is shifted to 1.35 MeV in the excitation curves for the α₂- and α₃-groups. The second maximum appears at 1.85 MeV in all curves. Angular distributions were measured at 7 energies between 1.0 and 2.2 MeV for the α₀- and α₂-transitions. The coefficients of the first four Legendre polinomials, describing these distributions, are given.

     

Ti掺杂对α″-Fe16N2相稳定性的影响

研究了掺杂Ti对α″-Fe₁₆N₂相稳定性的影响，发现适量Ti掺杂有利于α″-Fe₁₆N₂相的形成．理论分析表明，掺杂适量Ti元素后含Ti的α″-(Fe,Ti)₁₆N₂相的生成焓降低，使α″相的稳定性提高，也使α″相更易制备．Ti浓度为3—15at％的(FeTi)-N薄膜具有高饱和磁化强度，μ₀M_s=2.3—2.5T． 关键词：     

一系列薯蓣皂甙元-α-L鼠李糖基-(1→2)和(1→4)-β-D葡萄糖甙的1H和13C NMR归属

用同核和异核二维核磁共振方法全归属了一系列合成的薯蓣皂甙元-α-鼠李糖基-β-D葡萄糖甙的¹H和¹³C核磁共振谱线.这些薯蓣葡萄糖甙是薯蓣皂甙元-β-D葡萄糖甙(1),薯蓣皂甙元-α-L鼠李糖基(1→2)-β-D葡萄糖甙(2),薯蓣皂甙元-α-L鼠李糖基(1→4)-β-D葡萄糖甙(3),薯蓣皂甙元[-α-鼠李糖基-(→2)]-α-L鼠李糖基→-(1→4)-β-D葡萄糖甙(4)以及薯蓣皂甙元[-α-L鼠李糖基-(1→2)]-β-D阿拉伯糖基-(1→4)-β-D葡萄糖甙(5).     

Chemisorption of CO on tungsten (100): Combined flash desorption and electron stimulated desorption study. II

The chemisorption of CO on W(100) at ~ 100K has been studied using a combination of flash desorption and electron stimulated desorption (ESD) techniques. This is an extension of a similar study made for CO adsorption on W(100) at temperatures in the range 200–300K. As in the 200–300 K CO layer, both α₁-CO and α₂-CO are formed in addition to more strongly bound CO species upon adsorption at ~ 100K; the α-CO states yield CO⁺ and O⁺ respectively upon ESD. At low CO coverages, the α₁ and α₂-CO states are postulated to convert to β-CO or other strongly bound CO species upon heating. At higher CO coverages, α₁-CO converts to α₂-CO upon thermal desorption or electron stimulated desorption. There is evidence for the presence of other weakly-bound states in the low temperature CO layer having low surface concentration at saturation. The ESD behavior of the CO layer coadsorbed with hydrogen on W(100) is reported, and it is found that H(ads) suppresses either the concentration or the ionic cross section for α₁ and α₂-CO states.     

纳米晶永磁中面缺陷对畴壁钉扎机理的研究

畴壁钉扎模型的矫顽力可以表示为Hc=αpink2K1/μ0Ms-NeffMs，计算了微结构参数αpink随面缺陷内磁性参数A′和K′1的变化情况.结果表明，αpink可以在很宽的范围里取值.结合纳米单相Nd2Fe14B磁体，研究了晶粒边界的磁性参数和晶界厚度对αpink的影响，当A′/A=05，K′1/K1=01，以及晶界厚度r0＝332nm时，αpink最大.同时研究了纳米复相Nd2Fe14B/α-Fe磁体的αpink随α-Fe晶粒尺寸r0的变化情况，当r0＝7nm时，αpink最大. 关键词： 面缺陷 矫顽力 钉扎机理 纳米晶     

Sb incorporation at GaAs(0 0 1)-(2 × 4) surfaces

We examine the Sb incorporation and resulting surface reconstructions of Sb and GaSb deposited on GaAs(0 0 1). These films exhibit a mixed surface reconstruction of α2(2 × 4) and α(4 × 3). Initially, Sb reacts with Ga on the surface to form 2D islands of GaSb with an α(4 × 3) surface reconstruction. The 2D islands grow to a critical size of 30 nm², beyond which the atomic surface structure of the 2D island transforms to a α2(2 × 4) reconstruction in order to reduce the strain induced surface energy. This transformation is limited by the availability of Ga, which is necessary in higher quantities for the α2(2 × 4) reconstruction than for the α(4 × 3). The transformation results in a mixed α2(2 × 4)-α(4 × 3) surface where the surface reconstruction is coupled to the surface morphology, which may in the future provide a pathway for self-assembly of structures.     

高温快速固相烧结合成Zr1-xHfxW2O8的Raman光谱研究

首次采用高温快速固相烧结的方法合成了Zr1-x Hfx W2O8(x=0, 0.2, 0.3, 0.4, 0.5, 0.6, 1)固溶体。合适的合成条件为: 温度1573~1693 K, 时间10 min~1 h, 该方法使合成时间和能耗比传统固相反应烧结显著降低。Zr1-x Hfx W2O8的晶胞参数与晶胞体积随Hf4+含量的增加而减小。合成的样品晶粒尺寸比常规固相烧结合成样品的颗粒尺寸较小, 颗粒大小在1～10 μm之间。拉曼光谱分析表明, Zr1-xHfxW2O8(0相似文献   

Glycosylation patterns of human alpha2-macroglobulin: Analysis of lectin binding by electron microscopy

Human alpha2-macroglobulin (α2M) is a 720 kDa glycoprotein that presents two ultrastructural conformations: slow (S-α2M) and fast (F-α2M). α2M acts mainly as a proteinase scavenger, but an immunomodulatory role was also proposed. This work studies the effect of desialylation and deglycosylation on the structure patterns of α2M by ultrastructural analysis of lectin-induced aggregates, which represents a new approach that had never been previously used. Transmission electron microscopy (TEM) analysis showed the loss of S-α2M conformation after deglycosylation, indicating that glycosidic side-chains contribute to the molecular stability of S-α2M. TEM proved to be an important tool to analyze the effect of biochemical changes on α2M, yielding an objective qualitative control of its morphological state. Certain carbohydrate residues did not vary between the α2M conformations, since both bound similarly ConA and WGA lectins. However, the binding of PNA and BSI-B₄ was slightly lower in F-α2M than in S-α2M. Among the neuraminidases used to desialylate both conformations of α2M that from Arthrobacter ureafaciens was the most effective. Incubation with the lectins ConA or SNA, respectively specific for mannosyl and sialyl residues, led to dose-dependent patterns of aggregation of α2M molecules, mediated by lectin binding and clearly visualized by TEM.     

N-(6-甲基-2-苯并噻唑基)-α-氨基膦酸二乙酯的1H NMR研究

报道了N-(6-甲基-2-苯并噻唑基)-α-氨基膦酸二乙酯类化合物的¹H NMR数据,研究了α位苯环上取代基对α-CH的化学位移的影响.根据单晶结构确定了膦酸二乙酯的两个乙氧基的核磁不等价现象是由α位苯环的屏蔽作用造成的.研究了α位苯环上取代基对α位苯环的屏蔽作用的影响,并利用构象重叠方法解释了邻位取代基对屏蔽作用的影响.     

N-(6-甲基-2-苯并噻唑基)-α-氨基膦酸二乙酯的1H NMR研究

报道了N-(6-甲基-2-苯并噻唑基)-α-氨基膦酸二乙酯类化合物的¹H NMR数据,研究了α位苯环上取代基对α-CH的化学位移的影响.根据单晶结构确定了膦酸二乙酯的两个乙氧基的核磁不等价现象是由α位苯环的屏蔽作用造成的.研究了α位苯环上取代基对α位苯环的屏蔽作用的影响,并利用构象重叠方法解释了邻位取代基对屏蔽作用的影响.     

Dielectric behaviour of α-cyclodextrin,heptakis (2,3,6-tri-Omethyl)-β-cyclodextrin,randomly methylated β-cyclodextrin and low frequency Raman spectra of α- and β-cyclodextrins

The frequency and temperature dependence of the real (?′) and imaginary (?″)parts of the dielectric constant of α-cyclodrextrin (form 1; α-CD. 5.9H₂O) and α-cyclodextrin (form III; α-CD.7.6H₂O) and of the corresponding dried forms (α-CD.1.1H₂O, α-CD.2.9H₂O, respectively) has been investigated over the frequency range 0–100 k Hz and temperature range 130–350 K. In addition the dielectric behaviour has been investigated of heptakis-(2,3,6-tri-O-methyl)-β-cyclodextrin (β-CD.TRIME. 0.3H₂O) and randomly methylated β-cyclodextrin (β-CD.RAME.0.8H₂O). The dielectric behaviour is described well by Debyetype relaxation (α-disperson). All α-CD systems exhibit an additional ω-dispersion at low frequencies, which is attributed to proton transport. The fact that the ?′ values of α-CD form III are larger than those of α-CD form I is attributed to the different numbers and different strengths of the intramolecular hydrogen bonds. Form III has a stable conformation which is shown by the constant values of ?′ in the temperature range 125–250 K. By contrast, in form I the ?′ values increased linearly with temperature, indicating that the system passed through succesive conformations. The temperature dependence of ?″ and phase shift ∞ in all the specimens of α-CD (forms I, III) and fully methylated β-CD do not reveal any orderdisorder transition, because the developed hydrogen bonds ae not of the flip-flop type according to their crystal structures. The partially methylated β-CD reveals the characteristics of the order-disorder transition, which was observed before in the systems dried β-CD.2H₂O and non-dried β-CD.9.8H₂O. There is a direct relation between the hydroxyl groups of β-CD and the order-disorder transition. The order-disorder transition could also be shown in dried β-CD.2.4H₂O and non-dried β-CD.9.8H₂O samples but not in dried α-CD.1.1H₂O and non-dried a-CD.5.9H₂O samples, by low frequency Raman spectroscopy (< 180 cm^?1). The step-like temperature dependence of the band at 33.7cm^?1 reveals a transition at about 223K for both β-CD samples. In the case of α-CD samples the almost linear temperature dependence of the band at 49.1 cm^?1 does not reveal any transition.     

Determination of the strong coupling constant using available experimental data

We determine the strong coupling constant α s up to 4-loop in perturbative QCD.Testing QCD requires the measurement of α s over ranges of energy scales.In this analysis,the value of α s is determined from the unpolarized structure functions data points by minimizing the χ 2 function between the theory result and experimental data.Using perturbative QCD calculations from threshold corrections,we obtain α s (M 2 Z ) = 0.1139±0.0020 at N 3 LO which is in good agreement with the very recently results from the inclusive jet cross section in pp collisions at√ s=1.96 TeV.